Measurements Christos Leonidopoulos Columbia – DØ “Snowmass Studies” June 25, 2001.

Slides:



Advertisements
Similar presentations
LHCb-Babar Meeting 8 April Paul Soler University of Glasgow and Rutherford Appleton Laboratory A first look at B s J/ in LHCb.
Advertisements

Physics with antiprotons: CP violation in D-mesons Klaus Peters Ruhr-Universität Bochum KVI Groningen Jan 7, 2003.
Phenomenology of Charmless Hadronic B Decays Denis Suprun University of Chicago Thanks to C.-W. Chiang, M. Gronau, Z. Luo, J. Rosner for enjoyable collaborations.
Mixing at the B- Factories Daniel Marlow Princeton University Beauty /16/03 the “Iron City”
ITEP Meeting on the future of heavy flavour physics 1 Experimental methods for precise determination of CKM matrix sides Marie-Hélène Schune Member of.
CHARM-2007, Ithaca, NY Alexey Petrov (WSU) Alexey A. Petrov Wayne State University Table of Contents: Introduction CP-violation in charmed mesons Observables.
Search for B s oscillations at D  Constraining the CKM matrix Large uncertainty Precise measurement of V td  properly constrain the CKM matrix yield.
1 B s  J/  update Lifetime Difference & Mixing phase Avdhesh Chandra for the CDF and DØ collaborations Beauty 2006 University of Oxford, UK.
1 Charm Decays at Threshold Sheldon Stone, Syracuse University.
Measurements – Part II Christos Leonidopoulos Columbia/DØ -“Snowmass Studies” July 2, 2001 limiting theoretical & experimental errors expected sensitivity.
1 B Physics at CDF Junji Naganoma University of Tsukuba “New Developments of Flavor Physics“ Workshop Tennomaru, Aichi, Japan.
Iain Stewart MIT Iain Stewart MIT Nonleptonic Decays and the Soft Collinear Effective Theory Super B Factory Workshop, Hawaii, 2004.
Bs and Bd mixing Silas Hoffman and Georg Steinbrueck Introduction Current and future measurements B s mixing and physics beyond the SM.
B Decays to Open Charm (an experimental overview) Yury Kolomensky LBNL/UC Berkeley Flavor Physics and CP Violation Philadelphia, May 18, 2002.
B s and Λ b Lifetimes and BRs at the Tevatron Satyajit Behari (For the CDF Collab.) Johns Hopkins Univ., Baltimore,USA 25 th September 2006 Beauty 2006,
Study of CP violation in B s →J/ψ ϕ decay G.Borissov Lancaster University, UK.
2 July, 2001 Columbia D0 Snowmass Meeting - H.Evans 1 Exp. Systematic Errors Most CP measurements use time-dep rate asymmetries  a dir,mix = func’s of.
Chris Barnes, Imperial CollegeWIN 2005 B mixing at DØ B mixing at DØ WIN 2005 Delphi, Greece Chris Barnes, Imperial College.
Peter Fauland (for the LHCb collaboration) The sensitivity for the B S - mixing phase  S at LHCb.
B Production and Decay at DØ Brad Abbott University of Oklahoma BEACH 2004 June 28-July 3.
B 0 s  J/   LHC review Nicolò Magini University and INFN, Firenze For the ATLAS, CMS and LHCb collaborations Oxford, 28 th September 2006 Beauty 2006.
Discussion of B s oscillations and the recent  m s result from D0 LPHE meeting April 3, 2006 Olivier Schneider (EPFL) Presentation given at the LHCb Tuesday.
Donatella Lucchesi1 B Physics Review: Part II Donatella Lucchesi INFN and University of Padova RTN Workshop The 3 rd generation as a probe for new physics.
Measurement of CP violation with the LHCb experiment at CERN
A window for New Physics in B s →KK decays Joaquim Matias Universitat Autònoma de Barcelona David London & JM, PRD (2004) David London &JM & Javier Virto,
Introduction to Flavor Physics in and beyond the Standard Model
Wouter Verkerke, UCSB Limits on the Lifetime Difference  of Neutral B Mesons and CP, T, and CPT Violation in B 0 B 0 mixing Wouter Verkerke (UC Santa.
M. Adinolfi - University of Bristol1/19 Valencia, 15 December 2008 High precision probes for new physics through CP-violating measurements at LHCb M. Adinolfi.
RooFit toy MC sensitivity studies for  +  s and  m s from B s →D s  /K channels at LHCb Shirit Cohen NIKHEF MSc Colloquium May 11 th 2007.
NEW PHYSICS PHASE FROM CHARGINO YILI WANG IOWA STATE UNIVERITY SUPER B FACTORY WORKSHOP IN HAWAII JANUARY 19-22,2004.
CP violation measurements with the ATLAS detector E. Kneringer – University of Innsbruck on behalf of the ATLAS collaboration BEACH2012, Wichita, USA “Determination.
Gavril Giurgiu, Carnegie Mellon, FCP Nashville B s Mixing at CDF Frontiers in Contemporary Physics Nashville, May Gavril Giurgiu – for CDF.
1 Rare Bottom and Charm Decays at the Tevatron Dmitri Tsybychev (SUNY at Stony Brook) On behalf of CDF and D0 Collaborations Flavor Physics and CP-Violation.
Beautiful B Physics at the Tevatron IOP HEPP half day meeting Results From the Tevatron Imperial College London, 21 September 2005 Rick Jesik Imperial.
Penn CDF B Physics Overview Joseph Kroll – Penn DOE Site Visit – 8 August 2005.
Scatter Diagrams scatter plot scatter diagram A scatter plot is a graph that may be used to represent the relationship between two variables. Also referred.
Top quark IIHE Future interests  Towards data taking → new software  Have a broader physics output  Link theory-experiment  Calibration and.
Charm Physics Potential at BESIII Kanglin He Jan. 2004, Beijing
3/13/2005Sergey Burdin Moriond QCD1 Sergey Burdin (Fermilab) XXXXth Moriond QCD 3/13/05 Bs Mixing, Lifetime Difference and Rare Decays at Tevatron.
Sergey Burdin FNAL DØ Collaboration 8/12/2005 Chicago Flavor New Bs Mixing Result from DØ.
CHARM MIXING and lifetimes on behalf of the BaBar Collaboration XXXVIIth Rencontres de Moriond  March 11th, 2002 at Search for lifetime differences in.
Nouvelle physique dans le mixing des B d,s et approche frequentiste versus Bayesienne.
B 0 s  J/   with the ATLAS and CMS detectors Nicolò Magini University and INFN, Firenze Nagoya, 15 th December 2006 CKM th International Workshop.
1 Heavy Flavor Physics At the Tevatron Cheng-Ju S. Lin (Fermilab ) Aspen Winter Conference Aspen, Colorado 13 February 2006.
Mauro Donega’ - CDF collaboration meeting February 3, 2006 B d,s ->h 1 h 2 : BR, CP asymmetries, and lifetimes S. Budroni, S. Donati, M. Donega’, S. Giagu,
B hadrons Tevatron By Eduard De La Cruz Burelo University of Michigan On behalf of the CDF and D0 collaborations Lancaster University UK, 2-8.
Mike HildrethEPS/Aachen, July B Physics Results from DØ Mike Hildreth Université de Notre Dame du Lac DØ Collaboration for the DØ Collaboration.
B Production Cross Sections and Fragmentation Fractions at LHCb Laurence Carson (University of Santiago de Compostela) on behalf of the LHCb collaboration.
1 G. Sciolla – M.I.T. Beauty in the Standard Model and Beyond Palm tree and CKM Beauty in the Standard Model and Beyond Gabriella Sciolla (MIT) CIPANP.
Jeroen van Hunen (for the LHCb collaboration) The sensitivity to  s and  Γ s at LHCb.
G.P. Di Giovanni LPNHE - Univ. “Pierre et Marie Curie” - IN2P3/CNRS XLIIId Rencontres de Moriond EWK, 2008 B s Mixing,  s & CP Violation.
Marina Artuso WG1 CKM Status and future perspectives on V cs and V cd Marina Artuso Syracuse University.
Two Important Experimental Novelties: Dipartimento di Fisica di Roma La Sapienza Guido Martinelli Martina Franca 17/6/2007 Utfit & QCD in the Standard.
B s Mixing Parameters and the Search for CP Violation at CDF/D0 H. Eugene Fisk Fermilab 14th Lomonosov Conference Moscow State University August ,
Kinematics of Top Decays in the Dilepton and the Lepton + Jets channels: Probing the Top Mass University of Athens - Physics Department Section of Nuclear.
Niels Tuning (1) Topical lectures December 2010 CP violation Hour 3 N. Tuning.
Physics 222 UCSD/225b UCSB Lecture 7 Mixing & CP violation (3 of 3) Today, we focus on how to measure things, and what the present knowledge is from the.
CLEO-c Workshop 1 Data Assumptions Tagging Rare decays D mixing CP violation Off The Wall Beyond SM Physics at a CLEO Charm Factory (some food for thought)
C.D. LuCKM1  /  3 from Charmless B s Decays Cai-Dian Lü (IHEP, Beijing) Thanks A.Ali, G.Kramer and Li, Wang... Testing Uncertainty of.
C.D. LuMoriond1 Charmless hadronic B s Decays Cai-Dian Lü (IHEP, Beijing) Thanks Ali, Kramer and Li, Shen,Wang The study of hep-ph/
Latest CMS Results on ϕs
Patrick Robbe, LAL Orsay, 20 Nov 2013
Precision Probes for Physics Beyond the Standard Model
CP violation in the charm and beauty systems at LHCb
D0 Mixing and CP Violation from Belle
University of Tsukuba, Japan Particle Physics Phenomenology,
CP violation in Bs→ff and Bs → K*0K*0
Latest results on CP violation in B-meson mixing
B-physics at the LHC Beyond 2010, february
清华大学高能物理研究中心 Center for High Energy Physics, Tsinghua University
Presentation transcript:

measurements Christos Leonidopoulos Columbia – DØ “Snowmass Studies” June 25, 2001

Christos Leonidopoulos Mixing in the B system Since the t-diagram is the main contribution to the mixing    propagator        tcui iibis i ibis q m q VV mq VV,, * tc,u,i 22 * 1  We think we understand the mixing of B’s. A deviation from this simple diagram is a deviation from SM.

June 25, 2001Christos Leonidopoulos …Mixing in the B system If CP is a good symmetry in the B mixing… independent of CKM V ij elements ~5  (  30%) lattice QCD A measurement of one of ΔΓ, Δm is a SM prediction for the other

June 25, 2001Christos Leonidopoulos Experimental methods Fit of proper time distributions of untagged data samples: – large statistics – sensitivity ~ Fit of proper time distributions of CP eigenstates From the measurement of the BR of – reduced statistics – sensitivity ~

June 25, 2001Christos Leonidopoulos Measurements Assuming Without external constraints (expected within ±1%) PDG2001 LEP B-Oscillation Group (CDF not included) Phenomenology

June 25, 2001Christos Leonidopoulos Outlook Both expected to be measured by CDF and DØ (RunII) Phenomenology: hadronic uncertainties expected to be reduced (currently at 30%) Compare